000 03540nam a22005055i 4500
001 978-90-481-2433-6
003 DE-He213
005 20201213204215.0
007 cr nn 008mamaa
008 100301s2009 ne | s |||| 0|eng d
020 _a9789048124336
_9978-90-481-2433-6
024 7 _a10.1007/978-90-481-2433-6
_2doi
050 4 _aTA357-359
072 7 _aTGMF
_2bicssc
072 7 _aTGMF1
_2bicssc
072 7 _aTEC009070
_2bisacsh
072 7 _aSCI085000
_2bisacsh
082 0 4 _a620.1064
_223
100 1 _aZeytounian, R. Kh.
_eauthor.
245 1 0 _aConvection in Fluids
_h[electronic resource] /
_cby R. Kh. Zeytounian.
264 1 _aDordrecht :
_bSpringer Netherlands,
_c2009.
300 _aXV, 396 p.
_bonline resource.
336 _atext
_btxt
_2rdacontent
337 _acomputer
_bc
_2rdamedia
338 _aonline resource
_bcr
_2rdacarrier
347 _atext file
_bPDF
_2rda
490 1 _aFluid Mechanics and its Applications,
_x0926-5112 ;
_v90
505 0 _aShort Preliminary Comments and Summary of Chapters 2 to 10 -- The Navier—Stokes—Fourier System of Equations and Conditions -- The Simple Rayleigh (1916) Thermal Convection Problem -- The Bénard (1900, 1901) Convection Problem, Heated from below -- The Rayleigh—Bénard Shallow Thermal Convection Problem -- The Deep Thermal Convection Problem -- The Thermocapillary, Marangoni, Convection Problem -- Summing Up the Three Significant Models Related with the Bénard Convection Problem -- Some Atmospheric Thermal Convection Problems -- Miscellaneous: Various Convection Model Problems.
520 _aIn the present monograph, entirely devoted to “Convection in Fluids”, the purpose is to present a unified rational approach of various convective phenomena in fluids (mainly considered as a thermally perfect gas or an expansible liquid), where the main driving mechanism is the buoyancy force (Archimedean thrust) or temperature-dependent surface tension in homogeneities (Marangoni effect). Also, the general mathematical formulation (for instance, in the Bénard problem - heated from below)and the effect of the free surface deformation are taken into account. In the case of the atmospheric thermal convection, the Coriolis force and stratification effects are also considered. The main motivation is to give a rational, analytical, analysis of main above mentioned physical effects in each case, on the basis of the full unsteady Navier-Stokes and Fourier (NS-F) equations - for a Newtonian compressible viscous and heat-conducting fluid - coupled with the associated initiales (at initial time), boundary (lower-at the solid plane) and free surface (upper-in contact with ambiant air) conditions. This, obviously, is not an easy but a necessary task if we have in mind a rational modelling process with a view of a numerical coherent simulation on a high speed computer.
650 0 _aEngineering.
650 0 _aMathematics.
650 0 _aHydraulic engineering.
650 1 4 _aEngineering.
650 2 4 _aEngineering Fluid Dynamics.
650 2 4 _aEngineering Thermodynamics, Heat and Mass Transfer.
650 2 4 _aMathematical Modeling and Industrial Mathematics.
650 2 4 _aApplications of Mathematics.
710 2 _aSpringerLink (Online service)
773 0 _tSpringer eBooks
776 0 8 _iPrinted edition:
_z9789048124329
830 0 _aFluid Mechanics and its Applications,
_x0926-5112 ;
_v90
856 4 0 _uhttp://dx.doi.org/10.1007/978-90-481-2433-6
912 _aZDB-2-ENG
950 _aEngineering (Springer-11647)
999 _c24534
_d24534